TECHNICAL FIELD
[0001] The invention relates generally to optical cross-switches and more particularly to
a detector for monitoring signals in optical cross-switches.
BACKGROUND ART
[0002] In the past, telecommunications and data communications networks have traditionally
relied on electrical signals transmitted electrically on conductive lines. As higher
and higher data exchange rates are required, conductive lines are no longer sufficient
and increasingly the data is transmitted through the use of optical signals through
optical fibers. Equipment for efficiently generating and transmitting the optical
signals has been designed and implemented, but the manufacturability of optical switches
for use in telecommunications and data communications networks is problematic.
[0003] Fouquet et al. (USPN 5,699,462), which is assigned to the assignee of the present
invention, describes a switching matrix that is used for routing optical signals from
any one of a number of parallel input optical fibers to any one of a number of parallel
output optical fibers.
[0004] Referring now to FIG. 1 (PRIOR ART), therein is shown an isolated optical switching
element 10 formed on a substrate 12. The substrate 12 is of silicon or silica. The
optical switching element 10 includes planar waveguides defined by a lower cladding
layer 14, a core 16, and an upper cladding layer 18. The core 16 is primarily silicon
dioxide, but other materials that affect the index of refraction of the core may be
used. The cladding layers 14 and 18 are formed of a material having a refractive index
that is substantially different from the refractive index of the core material, so
that optical signals are guided along the core material.
[0005] In the manufacturing process, the core 16 is patterned to define an input waveguide
20 and an output waveguide 26 of a first waveguide path and to define an input waveguide
24 and an output waveguide 22 of a second waveguide path. The upper cladding layer
18 is then deposited over the core 16. A trench 28 is etched through the core 16 at
the intersection of the first and second waveguide paths and the two cladding layers
14 and 18 to the substrate 12. The waveguide paths intersect the trench 28 at an angle
of incidence greater than the critical angle of total internal reflection (TIR) when
the trench 28 is filled with a fluid, which can be a liquid, plasma, or a gas, having
a refractive index which closely matches the refractive index of the waveguides; thus,
light is transmitted to a "through" path to the output waveguide 26 when fluid is
present in the trench 28.
[0006] Thus, TIR diverts light from the input waveguide 20 at a region 27 to a "reflected"
path to the output waveguide 22, unless an index-matching fluid is located within
the gap between the aligned waveguides 20 and 26. The trench 28 is positioned in a
"forward" position with respect to the four waveguides 20, 26, 24, and 22 such that
one sidewall of the trench 28 passes through or is slightly offset from the intersection
of the axes of the waveguide paths on the side away from the input of the input waveguide
20.
[0007] Referring now to FIG. 2 (PRIOR ART), therein is shown a plurality of the optical
switching elements 10 in a 4 times 4 matrix 32. In the 4 times 4 matrix 32, any one
of four input waveguides 34, 36, 38 and 40 may be optically coupled to any one of
four output waveguides 42, 44, 46, and 48. The switching arrangement is referred to
as "non-blocking," since any free input waveguide can be connected to any free output
waveguide regardless of which connections have already been made through the switching
arrangement. Each of the sixteen optical switches has a trench that causes TIR in
the absence of an index-matching fluid at the gap between collinear waveguides, but
collinear waveguides of a particular waveguide path are optically coupled when the
gaps between the collinear waveguides are filled with the refractive index-matching
fluid. Trenches in which the waveguide gaps are filled with fluid are represented
by fine lines that extend at an angle through the intersections of optical waveguides
in the array. On the other hand, trenches in which the index-matching fluid is absent
at the gaps are represented by broad lines through a point of intersection.
[0008] For example, the input waveguide 20 of FIGS. 1 and 2 (PRIOR ART) is in optical communication
with the output waveguide 22 as a result of reflection at the empty gap of the trench
28. Since all other cross points for allowing the input waveguide 34 to communicate
with the output waveguide 44 are in a transmissive state, a signal that is generated
at the input waveguide 34 will be received at output waveguide 44. In like manner,
the input waveguide 36 is optically coupled to the first output waveguide 42, the
third input waveguide 38 is optically coupled to the fourth output waveguide 48, and
the fourth input waveguide 40 is coupled to the third output waveguide 46.
[0009] There are a number of available techniques for changing an optical switch of the
type shown in FIG. 1 from a transmissive state to a reflective state and back to the
transmissive state. One method of changing states involves forming and eliminating
the gap by forming and removing vapor bubbles in a refractive index-matching fluid.
A plurality of heating elements are used where the application of heat to a trench
forms the vapor bubble to remove the fluid and the removal of the heat causes the
vapor bubble to collapse and return the fluid. The heating elements and their control
are well known in the art and are used in ink jet printers.
[0010] The refractive index-matching fluid is supplied from a reservoir under the trench
and resides within the trench in the waveguide paths until a vapor bubble is formed
to create an index mismatch and cause light to be reflected at the sidewall of a trench.
Collapsing the vapor bubble returns the switch to the transmissive state. A bubble
forms in less than 1 ms when heat is applied and collapses in less than 1 ms when
heat is removed.
[0011] In the optical switching element 10, light coming in is from an independent outside
source and the light going out goes to an independent outside receiver, neither of
which can be tapped for information. Unlike an electrical circuit where it is possible
to make a parallel test connection, in optical circuits, parallel connections cause
losses in the signal. Further, an external coupler is required for each waveguide
and must be attached for each monitoring operation, which makes uninterrupted monitoring
of the optical switching element 10 costly and time consuming.
[0012] Those skilled in the art have long sought, with little success, a way to be able
to perform inexpensive uninterrupted monitoring of optical switches.
DISCLOSURE OF THE INVENTION
[0013] The present invention provides a method of monitoring a light signal in an optical
switch having a first waveguide and a second waveguide that intersect a first trench
such that optical coupling is dependent upon a fluid being at the first trench, and
having a test waveguide that intersects a second trench such that optical coupling
is dependent upon the fluid being at the second trench. By changing the fluid at the
first trench to switch the optical switch to cause a light signal to be reflected
from the first waveguide into the second waveguide and by partially changing the fluid
at the second trench to switch the optical switch to cause a portion of the light
signal to be reflected from the first waveguide into the test waveguide. The portion
of the light signal in the test waveguide can be monitored using a light monitor for
inexpensive uninterrupted monitoring of the optical switch.
[0014] The present invention further provides an optical switch for a light signal monitoring
system. The system includes a support structure having a first waveguide and a second
waveguide that intersect a first trench such that optical coupling is dependent upon
a fluid being at the first trench, and a test waveguide that intersects a second trench
such that optical coupling is dependent upon the fluid being at the second trench.
A mechanism is provided for changing the fluid at the first trench to switch the optical
switch to cause a light signal to be reflected from the first waveguide into the second
waveguide and a mechanism for partially changing the fluid at the second trench to
switch the optical switch to cause a portion of the light signal to be reflected from
the first waveguide into the test waveguide which can be monitored using a light monitor
for inexpensive uninterrupted monitoring of the optical switch.
[0015] The above and additional advantages of the present invention will become apparent
to those skilled in the art from a reading of the following detailed description when
taken in conjunction with the accompanying drawings.
BRIEF DESCRIPTION OF THE DRAWINGS
[0016]
FIG. 1 (PRIOR ART) is a top view of an optical switching element that utilizes total
internal reflection in accordance with the prior art;
FIG. 2 (PRIOR ART) is a 4 times 4 matrix of switching elements of FIG. 1 to allow
connection of any one of a number of input waveguides to any one of a number of output
waveguides in accordance with the prior art;
FIG. 3 is a 4 times 4 matrix of switching elements having a test column and test row
waveguides, which allow monitoring an optical cross-connect switch in a system in
accordance with the present invention.
BEST MODE FOR CARRYING OUT THE INVENTION
[0017] Referring now to FIG. 3, therein are shown a plurality of optical switching elements
110, 112, and 114 in a 4 times 4 matrix 132 on a support structure (not shown). In
the 4 times 4 matrix 132, any one of four input waveguides 134, 136, 138 and 140 may
be optically coupled to any one of four output waveguides 142, 144, 146, and 148.
The switching arrangement is referred to as "non-blocking," since any free input waveguide
can be connected to any free output waveguide regardless of which connections have
already been made through the switching arrangement. Each of the sixteen optical switches
has a trench that causes Total Internal Reflection (TIR) in the absence of an index-matching
fluid at the gap between collinear waveguides, but collinear waveguides of a particular
waveguide path are optically coupled when the gaps between the collinear waveguides
are filled with the refractive index-matching fluid. The trenches in which the waveguide
gaps are filled with fluid are represented by fine lines that extend at an angle through
the intersections of optical waveguides in the array. On the other hand, broad lines
through a point of intersection represent trenches in which the index-matching fluid
is absent at the gaps.
[0018] For example, the input waveguide 136 is in optical communication with the output
waveguide 144 as a result of reflection at the empty gap of a trench 150 in the optical
switching element 110. Since all other cross points for allowing the input waveguide
136 to communicate with the output waveguide 144 are in a transmissive state, a signal
that is generated for the input waveguide 136 will be output only at the output waveguide
144.
[0019] In the present invention, monitoring waveguides are present in the 4 times 4 matrix
132 in the form of a test column 152 and a test row 154 having associated trenches
in the same manner as the other waveguides. The test column 152 can have all "forward"
positioned trenches except for the trench at the intersection with the test row 154
or can have all "reversed" position trenches where the trenches pass through or are
slightly offset from the intersection of the axes of the waveguide paths toward the
input side of the input waveguides. The test row 154 has all "reversed" position trenches.
[0020] In developing the present invention, it was unexpectedly discovered that by using
a heater resistor for heating the fluid in a trench caused a change in its index of
refraction, which caused a partial mirroring effect. Further, it was observed that,
when a bubble begins to form, it forms as a sphere and moves up into the trench as
more vapor is formed as the fluid is brought to its boiling point by applying more
power to the heater resistor. The bubble squeezes against the front edge of the trench
and it has a rounded top on it. The rounded top first scatters light from the input
waveguide into the output waveguide. As the bubble grows, it starts to flatten in
the trench and to mirror the light. As the bubble grows fully, a full mirror effect
is established and the light from the input waveguide is fully reflected into the
output waveguide.
[0021] Using the test column 152 and the test row 154, it is has been found to be possible
to monitor any signal input by heating the fluid in a trench using the same resistor
used to form the switching bubble but by applying a much lower power. When the fluid
is heated, its index of refraction changes causing some of the signal to take a "switched"
path while the majority of the signal continues on the through path. Similarly, the
heating can also be controlled to produce a partial bubble, which also causes some
of the signal to take the switched path. The ability to control the heating to change
the refractive index and control the formation of the bubble allows control of the
degree of the TIR mirror effect. As a result, the signal may be "tapped" without a
significant signal loss.
[0022] A light receiver can monitor the tapped signal or monitor by being connected to either
the output of the test column 152 or of the test row 154.
[0023] For example, in unmonitored operation, the light signal is transmitted along the
input waveguide 136 where a bubble in the trench 150 causes reflection into the output
waveguide 144. To monitor the light signal in the input waveguide 136 and the output
waveguide 144, a bubble is formed at low power in a trench of a switching element
such as a trench 156 of the optical switching element 112 to direct a tapped signal
(shown as a dotted line) to a monitor 158.
[0024] As would be evident, monitoring could also be performed of any input waveguide by
forming a bubble at low power an appropriately positioned trench in the test column
152 to provide the tapped signal to an alternate monitor 160. Also, more than one
trench in the column 152 could be turned on at low power to monitor any activity into
the 4 times 4 matrix 132 without requiring scanning. Similarly, monitoring could also
be performed of any output waveguide using an appropriately positioned trench in the
test row 154 to provide the tapped signal to the monitor 158.
[0025] While the invention has been described in conjunction with a specific best mode,
it is to be understood that many alternatives, modifications, and variations will
be apparent to those skilled in the art in light of the aforegoing description. Accordingly,
it is intended to embrace all such alternatives, modifications, and variations that
fall within the spirit and scope of the included claims. All matters hither-to-fore
set forth or shown in the accompanying drawings are to be interpreted in an illustrative
and non-limiting sense.
1. A method of monitoring a light signal in a fluid containing device [132] comprising:
providing a fluid containing device [132] having a plurality of optical waveguides
[134,148,152] and a plurality of trenches [134-148, 134-152] provided therein, including:
a first waveguide [134] and a second waveguide [148] that intersect a first trench
[134-148] such that optical coupling between the first and second waveguides [134,148]
is dependent upon a fluid being at the first trench [134-148], and
a test waveguide [152] that intersects a second trench [134-152] such that optical
coupling between the test and first waveguides [152,134], is dependent upon the fluid
being at the second trench [134-152];
changing the fluid at the first trench [134-148] to switch the fluid containing device
[132] to cause a light signal to be reflected between the first and second waveguides
[134,148];
partially changing the fluid at the second trench [134-152] to switch the fluid containing
device [132] to cause a portion of the light signal to be reflected between the test
and first waveguides [152,134]; and
monitoring the portion of the light signal in the test waveguide [152] using a light
monitor [160].
2. The method as claimed in claim 1 wherein the fluid containing device [132] includes
a second test waveguide [154] that intersects a third trench [152-154] such that optical
coupling between the test waveguides [152,154] is dependent upon the fluid being at
the third trench [152-154] including:
changing the fluid at the third trench [152-154] to switch the fluid containing device
[132] to cause the portion of the light signal to be reflected from the test waveguide
[152] into the second test waveguide [154]; and wherein:
monitoring the portion of the light signal in the test waveguide [152] is performed
through the second test waveguide [154].
3. The method as claimed in claim 1 wherein the fluid containing device [132] includes
a third waveguide [146] that intersects a third trench [134-146] such that optical
coupling between the first and third waveguides [134,146] is dependent upon the fluid
being at the second trench [134-152] and a second test waveguide [154] intersects
a fourth trench [146-154] such that such that optical coupling between the second
test and third waveguides [154,146] is dependent upon the fluid being at the fourth
trench [146-154] including:
partially changing the fluid at the third trench [152-152] to switch the fluid containing
device [132] to cause the portion of the light signal to be reflected between the
first and third waveguides [134,146];
changing the fluid at the fourth trench [146-154] to switch the fluid containing device
[132] to cause the portion of the light signal to be reflected between the second
test and third waveguides [154,146]; and wherein:
monitoring the portion of the light signal in the third waveguide [146] is performed
through the second test waveguide [152].
4. The method as claimed in claim 1 wherein partially changing the fluid at the second
trench [134-152] changes the index of refraction thereof.
5. The method as claimed in claim 1 wherein partially changing the fluid at the second
trench [134-152] causes the beginning of bubble formation thereat.
6. A fluid containing device for a light signal monitoring system [132], comprising:
a support structure;
a plurality of optical waveguides [134,148,152] and a plurality of trenches [134-148,
134-152] provided in the support structure, including:
a first waveguide [134] and a second waveguide [148] that intersect a first trench
[134-148] such that optical coupling between the first and second waveguides [134,148]
is dependent upon a fluid being at the first trench [134-148], and
a test waveguide [152] that intersects a second trench [134-152] such that optical
coupling between the test and first waveguides [152,134], is dependent upon the fluid
being at the second trench [134-152];
a mechanism for changing the fluid at the first trench [134-148] to switch the fluid
containing device to cause a light signal to be reflected between the first and second
waveguides [134,148]; and
a mechanism for partially changing the fluid at the second trench [134-152] to switch
the fluid containing device [132] to cause a portion of the light signal to be reflected
between the test and first waveguides [152,134].
7. The fluid containing device as claimed in claim 6 including a second test waveguide
[154] that intersects a third trench [152-154] such that optical coupling between
the test waveguides [152,154] is dependent upon the fluid being at the third trench
[152-154] including:
a mechanism for changing the fluid at the third trench [152-154] to switch the fluid
containing device [132] to cause the portion of the light signal to be reflected from
the test waveguide [152] into the second test waveguide [154].
8. The fluid containing device as claimed in claim 6 including a third waveguide [146]
that intersects a third trench [134-146] such that optical coupling between the first
and third waveguides [134,146] is dependent upon the fluid being at the second trench
[134-152] and a second test waveguide [154] intersects a fourth trench [146-154] such
that such that optical coupling between the second test and third waveguides [154,146]
is dependent upon the fluid being at the fourth trench [146-154] including:
a mechanism for partially changing the fluid at the third trench [152-152] to switch
the fluid containing device [132] to cause the portion of the light signal to be reflected
between the first and third waveguides [134,146]; and
a mechanism changing the fluid at the fourth trench [146-154] to switch the fluid
containing device [132] to cause the portion of the light signal to be reflected between
the second test and third waveguides [154,146].
9. The fluid containing device as claimed in claim 6 wherein the mechanism for partially
changing the fluid at the second trench [134-152] changes the index of refraction
thereof.
10. The fluid containing device as claimed in claim 6 wherein the mechanism for partially
changing the fluid at the second trench [134-152] causes the beginning of bubble formation
thereat.